Zoom lens system, optical device with zoom lens system, and method of manufacturing zoom lens system

ABSTRACT

A zoom lens system comprises, in order from an object, a first lens group having a positive refractive power, a second lens group having a negative refractive power, and a third lens group having a positive refractive power. The first lens group has a first-a partial lens group and a first-b partial lens group arranged on an image side of the first-a partial lens group with an air space and is constructed such that the first-b partial lens group moves along an optical axis direction upon focusing from infinity to a close-range object. The third lens group is constituted by a third-a partial lens group having a positive refractive power and a third-b partial lens group having a negative refractive power arranged on the image side of the third-a partial lens group with an air space.

CROSS-REFERENCE TO RELATED APPLICATION

This application is a continuation of application Ser. No. 12/277,760filed Nov. 25, 2008 (now U.S. Pat. No. 7,889,439).

BACKGROUND OF THE INVENTION

1. Field of the Invention

The present invention relates to a zoom lens system used in an opticaldevice such as digital still camera.

2. Related Background Art

A positive-negative-positive zoom lens system has conventionally beenknown. This positive-negative-positive zoom lens system is constitutedby three lens groups of a first lens group having a positive refractivepower, a second lens group having a negative refractive power, and athird lens group having a positive refractive power in order from anobject. Upon zooming from a wide-angle end state (where the focal lengthis the shortest) to a telephoto end state (where the focal length is thelongest), the distance between the first lens group and the second lensgroup increases, the distance between the second lens group and thethird lens group decreases, and the first lens group moves toward theobject. For focusing, the first lens group as a whole is moved along theoptical axis (see, for example, Japanese Patent Publication No.2691563).

SUMMARY OF THE INVENTION

However, such a conventional zoom lens system has been problematic inthat, in the case where the lens group closest to the object as a wholeis used for focusing, the length of the zoom lens system becomes longerwhen adjusting a focus onto the close-range object. It has also beenproblematic in that the outer diameter of a lens in the zoom lens systembecomes greater in order to move the focal lens group along the opticalaxis.

In view of such problems, it is an object of the present invention toprovide a zoom lens system which has a small size and can attain highimaging performances while having a variable power ratio of about 3.5.

For purposes of summarizing the invention, certain aspects, advantages,and novel features of the invention have been described herein. It is tobe understood that not necessarily all such advantages may be achievedin accordance with any particular embodiment of the invention. Thus, theinvention may be embodied or carried out in a manner that achieves oroptimizes one advantage or group of advantages as taught herein withoutnecessary achieving other advantages as may be taught or suggestedherein.

In one aspect, the zoom lens system in accordance with the presentinvention comprises: in order from an object, a first lens group havinga positive refractive power; a second lens group having a negativerefractive power; and a third lens group having a positive refractivepower; wherein the first lens group has a first-a partial lens group anda first-b partial lens group arranged on an image side of the first-apartial lens group with an air space and is constructed such that thefirst-b partial lens group moves along an optical axis direction uponfocusing from infinity to a close-range object; wherein the third lensgroup comprises a third-a partial lens group having a positiverefractive power and a third-b partial lens group having a negativerefractive power arranged on the image side of the third-a partial lensgroup with an air space.

In another aspect, the zoom lens system in accordance with the presentinvention comprises, in order from an object: a first lens group havinga positive refractive power; a second lens group having a negativerefractive power; and a third lens group having a positive refractivepower; wherein the first lens group has a first-a partial lens group anda first-b partial lens group arranged on an image side of the first-apartial lens group with an air space and is constructed such that thefirst-b partial lens group moves along an optical axis direction uponfocusing from infinity to a close-range object; and wherein animage-side surface of a lens component arranged closest to an image isdistanced from an image plane by at least 10 mm but not more than 30 mm.

Preferably, the zoom lens system in accordance with the presentinvention is constructed such as to satisfy the following conditionalexpression:0.17<|f1b|/|f1a|<0.51where f1 a denotes a focal length of the first-a partial lens group, andf1 b denotes a focal length of the first-b partial lens group.

Preferably, the zoom lens system in accordance with the presentinvention is constructed such as to satisfy the following conditionalexpression:1.7<f1/fw<2.6where f1 denotes a focal length of the first lens group, and fw denotesa focal length of the whole system at a wide-angle end state.

Preferably, the zoom lens system in accordance with the presentinvention is constructed such as to satisfy the following conditionalexpression:1.15<|f1b|/f1<1.50where f1 denotes the focal length of the first lens group, and f1 bdenotes the focal length of the first-b partial lens group.

Preferably, in the zoom lens system in accordance with the presentinvention, the first-a partial lens group in the first lens group isstationary with respect to an image plane upon focusing from aclose-range object to infinity.

Preferably, in the zoom lens system in accordance with the presentinvention, the first-a partial lens group in the first lens group isconstructed such as to have a positive refractive power.

Preferably, in the zoom lens system in accordance with the presentinvention, the first-b partial lens group in the first lens group isconstructed such as to have a positive refractive power.

Preferably, the zoom lens system in accordance with the presentinvention is constructed such as to satisfy the following conditionalexpression:2.73<f1/(−f2)<6.20where f1 denotes the focal length of the first lens group, and f2denotes a focal length of the second lens group.

Preferably, the zoom lens system in accordance with the presentinvention is constructed such as to satisfy the following conditionalexpression:2.74<f1/f3<5.14where f1 denotes the focal length of the first lens group, and f3denotes a focal length of the third lens group.

Preferably, in the zoom lens system in accordance with the presentinvention, the third-b partial lens group in the third lens group iscomposed, in order from the object, of a cemented negative lens and anegative lens.

Preferably, in this case, the negative lens in the third-b partial lensgroup in the third lens group is a negative meniscus lens having aconvex surface facing the image.

Preferably, the zoom lens system in accordance with the presentinvention is constructed such that at least the first and third lensgroups move toward the object upon zooming from a wide-angle end stateto a telephoto end state.

Preferably, the zoom lens system in accordance with the presentinvention is constructed such that, upon zooming from a wide-angle endstate to a telephoto end state, a distance between the first and secondlens groups increases while a distance between the second and third lensgroups decreases.

The optical device in accordance with the present invention (e.g.,digital still camera 1 in accordance with an embodiment) is equippedwith any of the above-mentioned zoom lens systems forming an image ofthe object onto a predetermined image plane.

In one aspect, the method of manufacturing a zoom lens system inaccordance with the present invention comprises the steps of arranging,in order from an object, a first lens group having a positive refractivepower and including a first-a partial lens group and a first-b partiallens group arranged on an image side of the first-a partial lens groupwith an air space, a second lens group having a negative refractivepower, and a third lens group having a positive refractive power; andverifying a focusing action of moving the first-b partial lens groupalong an optical axis direction, the first-b partial lens group beingadapted to focus from infinity to a close-range object; wherein thethird lens group comprises a third-a partial lens group having apositive refractive power and a third-b partial lens group having anegative refractive power arranged on the image side of the third-apartial lens group with an air space; wherein the third-a partial lensgroup in the third lens group has; and wherein the third-b partial lensgroup in the third lens group has.

In another aspect, the method of manufacturing a zoom lens system inaccordance with the present invention comprises the steps of arranging,in order from an object, a first lens group having a positive refractivepower and including a first-a partial lens group and a first-b partiallens group arranged on an image side of the first-a partial lens groupwith an air space, a second lens group having a negative refractivepower, and a third lens group having a positive refractive power; andverifying a focusing action of moving the first-b partial lens groupalong an optical axis direction, the first-b partial lens group beingadapted to focus from infinity to a close-range object; wherein animage-side surface of a lens component arranged closest to the image isdistanced from an image plane by at least 10 mm but not more than 30 mm.

When the zoom lens system in accordance with the present invention andthe optical device equipped with the zoom lens system are constructed asin the foregoing, a zoom lens system having a small size and highimaging performances while exhibiting a high variable power ratio can berealized concerning a zoom lens system suitable for video cameras,digital still cameras, and the like using solid-state imaging devicesand the like.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 shows a refractive power arrangement of the zoom lens system inaccordance with an embodiment of the present invention;

FIG. 2 is a sectional view showing the structure of the zoom lens systemin accordance with Example 1;

FIG. 3A is an aberration chart in Example 1 in a wide-angle end stateupon focusing at infinity;

FIG. 3B is an aberration chart in Example 1 in an intermediate focallength state upon focusing at infinity;

FIG. 3C is an aberration chart in Example 1 in a telephoto end stateupon focusing at infinity;

FIG. 4 is a sectional view showing the structure of the zoom lens systemin accordance with Example 2;

FIG. 5A is an aberration chart in Example 2 in the wide-angle end stateupon focusing at infinity;

FIG. 5B is an aberration chart in Example 2 in the intermediate focallength state upon focusing at infinity;

FIG. 5C is an aberration chart in Example 2 in the telephoto end stateupon focusing at infinity;

FIG. 6 is a sectional view showing the structure of the zoom lens systemin accordance with Example 3;

FIG. 7A is an aberration chart in Example 3 in the wide-angle end stateupon focusing at infinity;

FIG. 7B is an aberration chart in Example 3 in the intermediate focallength state upon focusing at infinity;

FIG. 7C is an aberration chart in Example 3 in the telephoto end stateupon focusing at infinity;

FIG. 8 is a sectional view showing the structure of the zoom lens systemin accordance with Example 4;

FIG. 9A is an aberration chart in Example 4 in the wide-angle end stateupon focusing at infinity;

FIG. 9B is an aberration chart in Example 4 in the intermediate focallength state upon focusing at infinity;

FIG. 9C is an aberration chart in Example 4 in the telephoto end stateupon focusing at infinity;

FIG. 10 is a sectional view showing the structure of the zoom lenssystem in accordance with Example 5;

FIG. 11A is an aberration chart in Example 5 in the wide-angle end stateupon focusing at infinity;

FIG. 11B is an aberration chart in Example 5 in the intermediate focallength state upon focusing at infinity;

FIG. 11C is an aberration chart in Example 5 in the telephoto end stateupon focusing at infinity;

FIG. 12 is a sectional view showing the structure of the zoom lenssystem in accordance with Example 6;

FIG. 13A is an aberration chart in Example 6 in the wide-angle end stateupon focusing at infinity;

FIG. 13B is an aberration chart in Example 6 in the intermediate focallength state upon focusing at infinity;

FIG. 13C is an aberration chart in Example 6 in the telephoto end stateupon focusing at infinity;

FIG. 14A is a front view of an digital still camera mounted with thezoom lens system in accordance with an example of the present invention;

FIG. 14B is a rear view of the digital still camera mounted with thezoom lens system in accordance with the embodiment of the presentinvention;

FIG. 15 is a sectional view taken along the line A-A′ of FIG. 14A; and

FIG. 16 is a flowchart showing a method of manufacturing the zoom lenssystem in accordance with an embodiment of the present invention.

DESCRIPTION OF THE PREFERRED EMBODIMENTS

In the following, preferred embodiments of the present invention will beexplained with reference to the drawings. First, the structure of a zoomlens system ZL in accordance with an embodiment will be explained withreference to FIG. 2. This zoom lens system ZL comprises, in order froman object, a first lens group G1 having a positive refractive power, asecond lens group G2 having a negative refractive power, and a thirdlens group G3 having a positive refractive power. Upon zooming from thewide-angle end state (where the focal length is the shortest) to thetelephoto end state (where the focal length is the longest), at leastthe first lens group G1 and third lens group G3 move toward the objectso as to increase the distance between the first lens group G1 andsecond lens group G2 and decrease the distance between the second lensgroup G2 and third lens group G3. In the zoom lens system ZL, the firstlens group G1 is constituted by a first-a partial lens group G1 a and afirst-b partial lens group G1 b, while the first-b partial lens group G1b is arranged on the image side of the first-a partial lens group G1 awith an air space therebetween. This zoom lens system ZL can attain anexcellent imaging performance with a variable power ratio of about 3.5or higher.

Functions of the lens groups G1 to G3 will now be explained. The firstlens group G1 acts to converge luminous fluxes. In the wide-angle endstate, the first lens group G1 is arranged as close as possible to animage surface so that off-axis luminous fluxes pass therethrough on theoutside of the optical axis, whereby the lens diameter of the first lensgroup G1 is made smaller. In the telephoto end state, the first lensgroup G1 is moved toward the object so as to greatly increase thedistance from the second lens group G2, thus enhancing the convergingaction, whereby the length of the lens system is shortened.

In this embodiment, the first lens group G1 has the first-a partial lensgroup G1 a and the first-b partial lens group G1 b arranged on the imageside of the first-a partial lens group with an air space therebetween,and is constructed such that the first-b partial lens group G1 b movesalong an optical axis direction as indicated by an arrow in FIG. 2 uponfocusing from infinity to a close-range object. The black point shown inFIG. 2 indicates the in-focus state at infinity, and moves in thedirection of the depicted arrow when adjusting the focus onto theclose-range object, whereby focus adjustment is done. Such aconfiguration causes the first-b partial lens group G1 b to performfocusing while keeping the first-a partial lens group G1 a stationarywith respect to the image surface, thus minimizing the amount ofmovement upon focusing. Changes in performances caused by focusing arealso minimized.

The second lens group G2 acts to enlarge an image of the object formedby the first lens group G1. As the lens position state changes from thewide-angle end state to the telephoto end state, the distance betweenthe first lens group G1 and second lens group G2 is increased, so as toenhance the magnifying power, thereby changing the focal length.

The third lens group G3 acts to converge luminous fluxes expanded by thesecond lens group G2. For achieving higher performances, it will bepreferred if the third lens group G3 is constituted by a plurality oflens groups. The third lens group G3 also controls the exit pupilposition.

Based on the structure mentioned above, the zoom lens system ZL inaccordance with this embodiment is constructed such as to satisfy thefollowing conditional expression (1):0.17<|f1b|/f1a|<0.51  (1)where f1 a denotes a focal length of the first-a partial lens group G1a, and f1 b denotes a focal length of the first-b partial lens group G1b.

Conditional expression (1) is one for defining an appropriate range forthe ratio between focal lengths of the first-a partial lens group G1 aand first-b partial lens group G1 b in the first lens group G1. When theratio exceeds the upper limit of conditional expression (1), it isunfavorable in that the refractive power of the first-b partial lensgroup G1 b is so strong that the spherical aberration generated by thefirst lens group G1 alone becomes large. When the ratio is less than thelower limit of conditional expression (1), on the other hand, it isunfavorable in that the refractive power of the first-b partial lensgroup G1 b is so weak that the spherical aberration generated by thefirst lens group G1 alone is short of correction.

For securing the effects of this embodiment, it will be preferred if theupper limit of conditional expression (1) is 0.47. For securing theeffects of this embodiment more, it will be more preferred if the upperlimit of conditional expression (1) is 0.45. For securing the effects ofthis embodiment further, it will be further preferred if the upper limitof conditional expression (1) is 0.43 or 0.40. For securing the effectsof this embodiment, it will be preferred if the lower limit ofconditional expression (1) is 0.2. For securing the effects of thisembodiment more, it will be more preferred if the lower limit ofconditional expression (1) is 0.22. For securing the effects of thisembodiment further, it will be further preferred if the lower limit ofconditional expression (1) is 0.24.

Preferably, the zoom lens system ZL in accordance with this embodimentis constructed such as to satisfy the following conditional expression(2):1.7<f1/fw<2.6  (2)where f1 denotes a focal length of the first lens group G1, and fwdenotes a focal length of the whole system at a wide-angle end state.

Conditional expression (2) is one for defining an appropriate range forthe ratio between the focal length of the whole lens system and thefocal length of the first lens group G1 in the wide-angle end state.When the ratio exceeds the upper limit of conditional expression (2), itis unfavorable in that the refractive power of the first lens group isso weak that the spherical aberration generated by the first lens groupG1 alone is short of correction. It is also unfavorable in that thelength of the lens system becomes too long to achieve the object of theinvention. When the ratio is less than the lower limit of conditionalexpression (2), on the other hand, it is unfavorable in that therefractive power of the first lens group G1 is so strong that thespherical aberration generated by the first lens group G1 alone becomeslarge.

For securing the effects of this embodiment, it will be preferred if theupper limit of conditional expression (2) is 2.55. For securing theeffects of this embodiment more, it will be more preferred if the upperlimit of conditional expression (2) is 2.5. For securing the effects ofthis embodiment, it will be preferred if the lower limit of conditionalexpression (2) is 1.75. For securing the effects of this embodimentmore, it will be more preferred if the lower limit of conditionalexpression (2) is 1.8.

Preferably, the zoom lens system ZL in accordance with this embodimentis constructed such as to satisfy the following conditional expression(3):1.15<|f1b|/f1<1.50  (3)where f1 denotes the focal length of the first lens group G1, and f1 bdenotes the focal length of the first-b partial lens group f1 b.

Conditional expression (3) is one for defining an appropriate range forthe ratio between focal lengths of the first lens group G1 and first-bpartial lens group G1 b. When the ratio exceeds the upper limit ofconditional expression (3), the refractive power of the first-b partiallens group G1 b becomes weak. It is also unfavorable in that the amountof movement of focusing increases so much that the length of the lenssystem becomes longer, whereby the object of the present invention maynot be obtained. Further, coma fluctuates greatly at the time offocusing, whereby higher performances may not be achieved. When theratio is less than the lower limit of conditional expression (3), on theother hand, it is unfavorable in that the refractive power of thefirst-b partial lens group G1 b is so strong that the sphericalaberration and coma generated by the first lens group G1 alone becomelarge.

For securing the effects of this embodiment, it will be preferred if theupper limit of conditional expression (3) is 1.48. For securing theeffects of this embodiment more, it will be more preferred if the upperlimit of conditional expression (3) is 1.46. For securing the effects ofthis embodiment, it will be preferred if the lower limit of conditionalexpression (3) is 1.17. For securing the effects of this embodimentmore, it will be more preferred if the lower limit of conditionalexpression (3) is 1.19.

Preferably, in the zoom lens system ZL in accordance with thisembodiment, the first-a partial lens group G1 a in the first lens groupG1 is stationary with respect to the image surface when the lensposition state changes from a state focused at a short distance to astate focused at infinity, namely upon focusing from a close-rangeobject to infinity.

Preferably, in the zoom lens system ZL in accordance with thisembodiment, the first-a partial lens group G1 a in the first lens groupG1 has a positive refractive power in order to minimize fluctuations ofspherical aberration upon zooming and focusing.

Preferably, in the zoom lens system ZL in accordance with thisembodiment, the first-b partial lens group G1 b in the first lens groupG1 has a positive refractive power in order to minimize fluctuations ofspherical aberration upon zooming and focusing.

Preferably, the zoom lens system ZL in accordance with this embodimentsatisfies the following conditional expression (4):2.73<f1/(−f2)<6.20  (4)where f1 denotes the focal length of the first lens group, and f2denotes a focal length of the second lens group.

Conditional expression (4) is one for defining an appropriate range forthe ratio between focal lengths of the first lens group G1 and secondlens group G2. When the ratio exceeds the upper limit of conditionalexpression (4), the refractive power of the first lens group G1 becomesrelatively weak, so that the first lens group G1 fails to effectivelycontribute to varying power. Also, the amount of movement of the firstlens group G1 becomes large, thereby enhancing fluctuations of sphericalaberration occurring in the first lens group G1 at the time of zooming.As a result, performances are hard to keep from lowering in the wholezoom range from the wide-angle end state to the telephoto end state. Itis further unfavorable in that the refractive power of the second lensgroup G2 is relatively so strong that coma cannot be restrained fromoccurring, whereby high optical performances may not be obtained. Whenthe ratio is less than the lower limit of conditional expression (4), onthe other hand, the refractive power of the second lens group G2 becomesso weak that coma and field curvature are short of correction. It isalso unfavorable in that the second lens group G2 fails to effectivelycontribute to varying power, whereby a high variable power ratio of 3.5or more may not be secured.

For securing the effects of this embodiment, it will be preferred if theupper limit of conditional expression (4) is 6.0. For securing theeffects of this embodiment more, it will be more preferred if the upperlimit of conditional expression (4) is 5.8. For securing the effects ofthis embodiment, it will be preferred if the lower limit of conditionalexpression (4) is 2.9. For securing the effects of this embodiment more,it will be more preferred if the lower limit of conditional expression(4) is 3.1.

Preferably, the zoom lens system ZL in accordance with this embodimentsatisfies the following conditional expression (5):2.74<f1/f3<5.14  (5)where f1 denotes the focal length of the first lens group G1, and f3denotes a focal length of the third lens group G3.

Conditional expression (5) is one for defining an appropriate range forthe ratio between focal lengths of the first lens group G1 and thirdlens group G3. When the ratio exceeds the upper limit of conditionalexpression (5), it is unfavorable in that the refractive power of thethird lens group G3 is so weak that coma is hard to correct, wherebyhigh optical performances may not be obtained. When the ratio is lessthan the lower limit of conditional expression (5), on the other hand,it is unfavorable in that the refractive power of the third lens groupG3 is so strong that spherical aberration is corrected in excess.

For securing the effects of this embodiment, it will be preferred if theupper limit of conditional expression (5) is 5.0. For securing theeffects of this embodiment more, it will be more preferred if the upperlimit of conditional expression (5) is 4.8. For securing the effects ofthis embodiment, it will be preferred if the lower limit of conditionalexpression (5) is 3.4. For securing the effects of this embodiment more,it will be more preferred if the lower limit of conditional expression(5) is 3.2.

For further higher performances, it will be preferred in the zoom lenssystem ZL in accordance with this embodiment if the third lens group G3is constructed as follows. That is, for favorably correcting thespherical aberration, coma, and field curvature generated by the thirdlens group G3 alone, the third lens group G3 is preferably constitutedby a third-a partial lens group G3 a and a third-b partial lens group G3b arranged on the image side of the third-a partial lens group G3 a withan air space therebetween. Here, the third-a partial lens group G3 a andthird-b partial lens group G3 b are separated from each other by a gapyielding the widest air space between lenses within the third lens groupG3.

For further higher performances and smaller size, it will be preferredin the zoom lens system ZL in accordance with this embodiment if thethird lens group G3 is constructed as follows. That is, for favorablycorrecting the spherical aberration, coma, and field curvature generatedby the third lens group G3 alone, the third-a and third-b partial lensgroups G3 a, G3 b have positive and negative refractive powers,respectively. Thus placing third-a and third-b partial lens groups G3 a,G3 b in an appropriate refractive power arrangement can contribute toshortening the length of the lens system and distancing the exit pupil.

Preferably, in this case, the third-b partial lens group G3 b has twonegative lens components. More preferably, all the lens componentsincluded in the third-b partial lens group G3 b have a negativerefractive power. Such a configuration can adjust the position of theexit pupil of the zoom lens system ZL, so as to prevent darkness(shading) from occurring at corners of a taken picture and shorten thelength of the zoom lens.

Preferably, the zoom lens system ZL in accordance with this embodimentis a so-called telephoto zoom lens system including long focal lengthssuch as about 80 mm at the wide-angle end and about 300 mm at thetelephoto end in terms of 35-mm film format. More preferably, the zoomlens system ZL in accordance with this embodiment has a variable powerratio of about 3 to 4. More preferably, in the zoom lens system ZL inaccordance with this embodiment, the distance from the image-sidesurface of the lens component arranged closest to the image to the imagesurface in the shortest state (the wide-angle end state in each ofexamples which will be explained later) is about 10 to 30 mm.

For further higher performances, it will be preferred in the zoom lenssystem ZL in accordance with this embodiment if the third lens group G3is constructed as follows. That is, for favorably correcting coma anddistancing the exit pupil, the third lens group is preferablyconstituted by a cemented negative lens and a negative meniscus lenshaving a convex surface facing the image in order from the object.

For further higher performances, it will be preferred in the zoom lenssystem ZL in accordance with this embodiment if the first lens group G1is constructed as follows. That is, one of the first-a partial lensgroup G1 a and first-b partial lens group G1 b in the first lens groupG1 is preferably a single lens component, while the other is morepreferably a cemented lens component. Such a configuration allows thecemented lens component to correct chromatic aberration. This can alsoevade fluctuations in chromatic aberration which may occur when movingthe lens group if each of the partial lens groups is a cemented lenscomponent, and reduce the weight of the first lens group. Morepreferably, the number of lens components constituting the first lensgroup G1 is 3 or less.

An outline of a method of manufacturing the zoom lens system will now beexplained with reference to FIG. 16.

To begin with, the first lens group G1, second lens group G2, and thirdlens group G3 of this embodiment are built into a cylindrical lensbarrel. The lens groups may be built into the lens barrel one by one intheir order along the optical axis, or a part or all of the lens groupsmay be integrally held with a holding member and then assembled with alens barrel member. Preferably, after the lens groups are built into thelens barrel, it is determined whether or not an image of an object isformed in the state where the lens groups are built in the lens barrel.

After the zoom lens system is assembled as mentioned above, its variousactions are verified. Examples of the actions include a focusing actionin which the first-a partial lens group G1 b for adjusting a focus frominfinity to the close-range object moves along the optical axis, avarying power action in which at least a part of lens groups moves alongthe optical axis when varying power, and a camera shake correctingaction in which at least a part of lenses moves so as to have acomponent orthogonal to the optical axis. When varying power from thewide-angle end state to the telephoto end state in this embodiment, atleast the first and third lens groups move toward the object such as toincrease the distance between the first and second lens groups anddecrease the distance between the second and third lens groups. Thevarious actions can be verified in any order.

The optical device in accordance with an embodiment will now beexplained. This optical device is an optical device equipped with a zoomlens system for forming an image of an object onto a predetermined imagesurface, wherein the zoom lens system is constituted by the zoom lenssystem ZL in accordance with the embodiment.

FIGS. 14A, 14B, and 15 show the structure of an digital still camera(hereinafter simply referred to as camera) 1 as an optical devicedetachably equipped with the above-mentioned zoom lens system ZL. Whenan undepicted power button is pressed in this camera 1, an undepictedshutter of its shooting lens system (zoom lens system ZL) is released,so that light from an undepicted object is converged by the zoom lenssystem ZL, so as to form an image on an imaging device C (e.g., CCD orCMOS) arranged at an image surface I. The object image formed on theimaging device C is displayed on a liquid crystal monitor 2 arrangedbehind the camera 1. After deciding a composition of the object imagewhile viewing the liquid crystal monitor 2, a photographer pushes down arelease button 3, so as to capture the object image with the imagingdevice C and record it into an undepicted memory for storage.

Arranged in the camera 1 are an auxiliary light emitting part 4 foremitting auxiliary light when the object is dark, a wide (W)—telephoto(T) button 5 for zooming the zoom lens system ZL from the wide-angle endstate (W) to the telephoto end state (T), a function button 6 used forsetting various conditions and the like of the camera 1, and the like.

Though the above explanations and examples which will follow illustratethe zoom lens system ZL having a three-group structure, the foregoingstructural conditions and the like are also applicable to other groupstructures such as those composed of four and five groups. For example,while the lens system is constructed by three movable groups in thisembodiment, additional lens groups may be inserted between the existinglens groups or arranged adjacent thereto on the image side or objectside. The lens groups refers to parts, separated from each other by anair space which varies at the time of varying power, each having atleast one lens.

A single or plurality of lens groups or partial lens groups may be movedin the optical axis direction as a focusing lens group for focusing froman object at infinity to a close-range object. In this case, thefocusing lens group is employable for autofocusing and suitable forbeing driven with a motor (such as ultrasonic motor) for autofocusing.It will be preferred in particular if at least a part of the first lensgroup is employed as the focusing lens group.

In order to prevent shooting from failing because of image blurs causedby camera shakes and the like which are likely to occur in a zoom lenssystem having a high variable power, the present invention can combine ashake detection system for detecting shakes of the lens system anddriving means with the lens system and drive the whole or part of one ofthe lens groups constituting the lens system as a vibration reductionlens with the driving means such that the vibration reduction lens groupis decentered so as to correct image blurs (fluctuations in the imagesurface position) due to shakes of the lens system detected by the shakedetection system, thus shifting the image, thereby correcting the imageblurs. It will be preferred in particular if the second lens group G2 asa whole is the vibration reduction lens group. Thus, the zoom lenssystem ZL in accordance with this embodiment can function as a so-calledvibration reduction optical system. In this embodiment, however, thelenses within the third lens group G3 move only in directions parallelto the optical axis. That is, the third lens group G3 in this embodimenthas no lenses which move in directions perpendicular to the optical axisand thus fails to function as a vibration reduction optical system.

The lens surfaces may be formed spherical, planar, or aspherical. Thespherical or planar lens surfaces are favorable in that processing oflenses and adjustment of their assembling are easy, so as to preventoptical performances from deteriorating because of errors in theprocessing and adjustment of assembling. They are also favorable in thatdepicting performances deteriorate less even when the image surface isshifted. On the other hand, the aspherical lens surfaces may be any ofthose made by grinding, glass-molded aspherical surfaces in which glassis formed aspherical with molds, and composite aspherical surfaces inwhich a resin is formed aspherical on a surface of glass. The lenssurfaces may also be diffractive surfaces. The lenses may begradient-index lenses (GRIN lenses) or plastic lenses.

Though an aperture stop S is preferably arranged near the third lensgroup G3 (near the third-a partial lens group G3 a when the third lensgroup G3 is constituted by the third-a partial lens group G3 a andthird-b partial lens group G3 b), a lens frame may act therefor withoutproviding any member as the aperture stop.

When an antireflection coating exhibiting high transmittance over abroad wavelength range is applied to each lens surface, flares andghosts can be reduced, so as to achieve high optical performances with ahigh contrast.

The present invention is explained with reference to constituentfeatures of its embodiments for easier understanding, but is not limitedthereto as a matter of course.

EXAMPLES

Examples of the present invention will now be explained with referenceto the accompanying drawings. FIG. 1 shows the refractive powerdistribution of the zoom lens system ZL in accordance with the examplesand how its lens groups move upon zooming from the wide-angle end state(W) to the telephoto end state (T). As shown in FIG. 1, the zoom lenssystem ZL in accordance with the examples is composed, in order from theobject, of the first lens group G1 having a positive refractive power,the second lens group G2 having a negative refractive power, and thethird lens group G3 having a positive refractive power, and a filtergroup FL comprising a low-pass filter, an infrared cut filter, and thelike. Upon zooming from the wide-angle end state to the telephoto endstate, at least the first lens group G1 and third lens group G3 movetoward the object. The examples are constructed such that, upon zoomingfrom the wide-angle end state to the telephoto end state, the distancebetween the first lens group G1 and second lens group G2 increases whilethe distance between the second lens group G2 and third lens group G3decreases.

In Example 4, the aspherical surface is represented by the followingexpression (a):S(y)=(y ² /r)/[1+(1−κ×y ² /r ²)^(1/2) ]+A4×y ⁴ +A6×y ⁶ +A8×y ⁸ +A10×y¹⁰  (a)where y denotes the height perpendicular to the optical axis, S(y)denotes the distance (sag amount) along the optical axis from thetangent plane at the vertex of the aspherical surface to the asphericalsurface at the height y, r denotes the radius of curvature of areference spherical surface (radius of paraxial curvature), κ denotesthe conical constant, and An denotes the nth-order asphericalcoefficient. “E-n” (where n is an integer) denotes “×10^(−n)” in Example4 which will be set forth later.

In Example 4, the second-order aspherical surface coefficient A2 is 0.In the table for Example 4, “*” is added to the left side of the surfacenumber representing the aspherical surface.

Example 1

FIG. 2 is a view showing the structure of the zoom lens system ZL1 inaccordance with Example 1 of the present invention. In the zoom lenssystem ZL1 of FIG. 2, the first lens group G1 is composed, in order fromthe object, of a first-a partial lens group G1 a and a first-b partiallens group G1 b; the first-a partial lens group G1 a is made of acemented positive lens constructed by cementing a negative meniscus lensL11 having a convex surface facing the object and a double convex lensL12 together; and the first-b partial lens group G1 b is constituted bya double convex lens L13. The second lens group G2 is composed, in orderfrom the object, of a double concave lens L21, a cemented negative lensconstructed by cementing a double concave lens L22 and a double convexlens L23 together, and a double concave lens L24. The third lens groupG3 is composed, in order from the object, of a third-a partial lensgroup G3 a and a third-b partial lens group G3 b; the third-a partiallens group G3 a is composed of a double convex lens L31, a cementednegative lens constructed by cementing a double convex lens L32 and adouble concave lens L33 together, and a double convex lens L34; and thethird-b partial lens group G3 b is composed of a cemented negative lensconstructed by cementing a double concave lens L35 and a double convexlens L36 together and a negative meniscus lens L37 having a concavesurface facing the object. Further, a filter group FL is constructed bya low-pass filter, an infrared cut filter, and the like.

An image surface I is formed on an imaging device which is not depicted,while the imaging device is constituted by CCD, CMOS, and the like (asin examples which will follow). An aperture stop S is arranged closestto the object in the third lens group G3, and moves together with thethird lens group G3 at the time of zooming from the wide-angle end stateto the telephoto end state.

The following Table 1 lists values of data in Example 1. In Table 1, f,F.NO, 2ω), and Bf denote the focal length, f-number, angle of view, andback focus, respectively. The surface number indicates the lens surfacenumber counted in order from the object along the advancing direction oflight beams, while the refractive index and Abbe number refer to theirvalues at d-line (λ=587.6 nm). While “mm” is generally used for the unitof lengths such as focal length f, radius of curvature r, and surfacedistance d listed in all of the following data values, the unit is notlimited thereto, since optical systems can attain similar opticalperformances even after being proportionally enlarged or reduced. Theradius of curvature of 0.0000 indicates a plane, while the refractiveindex of air, which is 1.00000, is omitted. These explanations ofsymbols and data tables also apply to examples which will follow. In thefollowing tables, W, IFL, T, IH, and TLL denote the Wide-angle end,Intermediate focal length, Telephoto end, Image height, and Total lenslength, respectively. Also, s, r, d, n, and v denote the Surface No.,Radius of curvature, Surface distance, Refractive index, and Abbenumber, respectively, in the following tables.

TABLE 1 W IF T f = 30.00 ~ 65.50 ~ 107.09 F.NO = 4.14 ~ 4.85 ~ 5.75 2ω =31.89 ~ 14.24 ~ 8.79 IH = 8.50 ~ 8.50 ~ 8.50 TLL = 76.00 ~ 95.28 ~105.00 s r d n ν 1 280.8182 0.95 1.83400 37.16 2 51.9013 3.00 1.4978282.52 3 69.7458 4.20 4 39.2708 2.35 1.49782 82.52 5 −1873.4179 (d5) 6−150.2667 0.80 1.69680 55.53 7 30.0997 0.85 8 −29.0467 0.80 1.6968055.53 9 18.3923 2.20 1.84666 23.78 10 −166.9992 1.00 11 −20.5558 0.801.72916 54.68 12 4007.8031 (d12) 13 0.0000 0.50 (aperture stop S) 1475.9842 2.15 1.60311 60.64 15 −23.7528 0.10 16 20.7865 3.30 1.4978282.52 17 −15.5285 0.80 1.80384 33.89 18 77.1180 0.10 19 13.9597 2.701.60300 65.44 20 −83.0727 8.55 21 −29.0384 0.80 1.74400 44.79 22 6.75513.75 1.61293 37.00 23 −16.0409 0.85 24 −8.2498 1.15 1.78800 47.37 25−13.8878 (d25) 26 0.0000 1.00 1.51680 64.12 27 0.0000 1.50 28 0.00001.87 1.51680 64.12 29 0.0000 0.40 30 0.0000 0.70 1.51680 64.12 31 0.0000(Bf) Focal length of lens group Group Initial surface Focal length 1 160.6470 2 6 −12.6602 3 14 14.7906

In Example 1, the axial air space d5 between the first and second lensgroups G1, G2, the axial air space d12 between the second and third lensgroups G2, G3, the axial air space d25 between the third lens group G3and filter group FL, and the back focus Bf vary during zooming. Thefollowing Table 2 lists variable spaces at infinity at respective focallengths in the wide-angle end, intermediate focal length, and telephotoend states.

TABLE 2 W IF T f 30.0001 65.5002 107.0904 d5 1.9728 19.9502 25.5252 d129.7735 5.1106 1.6047 d25 16.6581 22.6196 30.2744 Bf 0.5000 0.5001 0.5002

The following Table 3 lists values corresponding to the conditionalexpressions in Example 1.

TABLE 3 fw = 30.0001 f1 = 60.6470 f1a = 271.7971 f1b = 77.2975 f2 =−12.6602 f3 = 14.7906 (1) f1b/f1a = 0.2844 (2) f1/fw = 2.0216 (3) f1b/f1= 1.2745 (3) f1/(−f2) = 4.7904 (3) f1/f3 = 4.1004

FIGS. 3A to 3C are aberration charts showing various aberrations ofExample 1 at d-line (λ=587.6 nm). FIG. 3A is an aberration chart uponfocusing at infinity in the wide-angle end state (f=30.00 mm) FIG. 3B isan aberration chart upon focusing at infinity in the intermediate focallength state (f=65.50 mm). FIG. 3C is an aberration chart upon focusingat infinity in the telephoto end state (f=107.09 mm).

In each aberration chart, FNO and A denote the f-number and the halfangle of view at each image height, respectively. In each astigmatismchart, solid and broken lines indicate sagittal and meridional imagesurfaces, respectively. The same symbols as those of this example willbe used in various aberration charts of the following examples. Theaberration charts indicate that various aberrations are favorablycorrected in each focal length state from the wide-angle end state tothe telephoto end state, whereby Example 1 has excellent imagingperformances.

Example 2

FIG. 4 is a view showing the structure of the zoom lens system ZL2 inaccordance with Example 2 of the present invention. In the zoom lenssystem ZL2 of FIG. 4, the first lens group G1 is composed, in order fromthe object, of a first-a partial lens group G1 a and a first-b partiallens group G1 b; the first-a partial lens group G1 a is made of acemented positive lens constructed by cementing a negative meniscus lensL11 having a convex surface facing the object and a double convex lensL12 together; and the first-b partial lens group G1 b is constituted bya positive meniscus lens L13 having a convex surface facing the object.The second lens group G2 is composed, in order from the object, of acemented negative lens constructed by cementing a positive meniscus lensL21 having a concave surface facing the object and a double concave lensL22 together and a negative meniscus lens L23 having a concave surfacefacing the object. The third lens group G3 is composed, in order fromthe object, of a third-a partial lens group G3 a and a third-b partiallens group G3 b; the third-a partial lens group G3 a is composed of apositive meniscus lens L31 having a concave surface facing the object, acemented positive lens constructed by cementing a double convex lens L32and a double concave lens L33 together, and a double convex lens L34;and the third-b partial lens group G3 b is composed of a cementednegative lens constructed by cementing a double concave lens L35 and adouble convex lens L36 together and a negative meniscus lens L37 havinga concave surface facing the object. Further, a filter group FL isconstructed by a low-pass filter, an infrared cut filter, and the like.An aperture stop S is arranged closest to the object in the third lensgroup G3, and moves together with the third lens group G3 at the time ofzooming from the wide-angle end state to the telephoto end state.

The following Table 4 lists values of data in Example 2.

TABLE 4 W IF T f = 30.00 ~ 71.50 ~ 107.09 F.NO = 4.21 ~ 5.04 ~ 5.68 2ω =31.94 ~ 13.08 ~ 8.80 IH = 8.50 ~ 8.50 ~ 8.50 TLL = 85.00 ~ 100.37 ~105.00 s r d n ν 1 240.0450 0.95 1.83400 37.16 2 57.2707 3.00 1.4978282.52 3 −78.0810 4.96 4 45.8457 3.39 1.49782 82.52 5 2463.4485 (d5) 6−51.4985 1.78 1.84666 23.78 7 −17.8534 0.80 1.56384 60.66 8 28.7811 1.509 −16.9251 0.80 1.62041 60.29 10 −301.4407 (d10) 11 0.0000 0.50(aperture stop S) 12 −401.0383 1.66 1.49700 81.54 13 −35.3632 0.10 1425.0498 3.08 1.60300 65.44 15 −15.7224 0.80 1.80384 33.89 16 203.83410.33 17 17.4417 2.36 1.61800 63.33 18 −126.1678 9.45 19 −130.2123 0.801.83481 42.71 20 8.3229 3.10 1.62004 36.26 21 −21.3280 2.50 22 −10.05161.20 1.78800 47.37 23 −17.1063 (d23) 24 0.0000 1.00 1.51680 64.12 250.0000 1.50 26 0.0000 1.87 1.51680 64.12 27 0.0000 0.40 28 0.0000 0.701.51680 64.12 29 0.0000 (Bf) Focal length of lens group Group Initialsurface Focal length 1 1 69.0008 2 6 −17.7314 3 12 19.4587

In Example 2, the axial air space d5 between the first and second lensgroups G1, G2, the axial air space d10 between the second and third lensgroups G2, G3, the axial air space d23 between the third lens group G3and filter group FL, and the back focus Bf vary during zooming. Thefollowing Table 5 lists variable spaces at infinity at respective focallengths in the wide-angle end, intermediate focal length, and telephotoend states.

TABLE 5 W IF T f 30.0000 71.4999 107.0900 d5 2.8000 21.7359 26.5682 d1017.4541 7.0722 1.5000 d23 15.7213 22.5407 27.9069 Bf 0.4999 0.50010.5002

The following Table 6 lists values corresponding to the conditionalexpressions in Example 2.

TABLE 6 fw = 30.0000 f1 = 69.0008 f1a = 249.4035 f1b = 93.7955 f2 =−17.7314 f3 = 19.4587 (1)f1b/f1a = 0.3761 (2)f1/fw = 2.3000 (3)f1b/f1 =1.3593 (4)f1/(−f2) = 3.8915 (5)f1/f3 = 3.5460

FIGS. 5A to 5C are aberration charts showing various aberrations ofExample 2 at d-line (λ=587.6 nm). FIG. 5A is an aberration chart uponfocusing at infinity in the wide-angle end state (f=30.00 mm) FIG. 5B isan aberration chart upon focusing at infinity in the intermediate focallength state (f=71.50 mm). FIG. 5C is an aberration chart upon focusingat infinity in the telephoto end state (f=107.09 mm) The aberrationcharts indicate that various aberrations are favorably corrected in eachfocal length state from the wide-angle end state to the telephoto endstate, whereby Example 2 has excellent imaging performances.

Example 3

FIG. 6 is a view showing the structure of the zoom lens system ZL3 inaccordance with Example 3 of the present invention. In the zoom lenssystem ZL3 of FIG. 6, the first lens group G1 is composed, in order fromthe object, of a first-a partial lens group G1 a and a first-b partiallens group G1 b; the first-a partial lens group G1 a is made of acemented positive lens constructed by cementing a negative meniscus lensL11 having a convex surface facing the object and a double convex lensL12 together; and the first-b partial lens group G1 b is constituted bya double convex lens L13. The second lens group G2 is composed, in orderfrom the object, of a double concave lens L21, a cemented negative lensconstructed by cementing a double concave lens L22 and a double convexlens L23 together, and a double concave lens L24. The third lens groupG3 is composed, in order from the object, of a third-a partial lensgroup G3 a and a third-b partial lens group G3 b; the third-a partiallens group G3 a is composed of a double convex lens L31, a cementedpositive lens constructed by cementing a double convex lens L32 and adouble concave lens L33 together, and a double convex lens L34; and thethird-b partial lens group G3 b is composed of a cemented negative lensconstructed by cementing a double concave lens L35 and a double convexlens L36 together and a negative meniscus lens L37 having a concavesurface facing the object. Further, a filter group FL is constructed bya low-pass filter, an infrared cut filter, and the like. An aperturestop S is arranged closest to the object in the third lens group G3, andmoves together with the third lens group G3 at the time of zooming fromthe wide-angle end state to the telephoto end state.

The following Table 7 lists values of data in Example 3.

TABLE 7 W IF T f = 29.54 ~ 65.50 ~ 107.09 F. NO = 4.11 ~ 4.87 ~ 5.77 2ω= 32.41 ~ 14.23 ~ 8.79 IH = 8.50 ~ 8.50 ~ 8.50 TLL = 75.50 ~ 95.08 ~105.00 s r d n ν 1 234.2875 0.95 1.83400 37.16 2 47.9733 3.00 1.4978282.52 3 −67.6099 3.99 4 39.4608 2.40 1.49782 82.52 5 −1268.7397 (d5) 6−118.4337 0.80 1.75500 52.32 7 35.2574 0.90 8 −38.6035 0.80 1.7200050.23 9 14.0729 2.15 1.84666 23.78 10 −1793.3532 1.00 11 −19.9098 0.801.75500 52.32 12 287.2798 (d12) 13 0.0000 0.50 (aperture stop S) 14130.0681 2.20 1.49782 82.52 15 −21.0703 0.10 16 25.0108 3.50 1.6030065.44 17 −13.7558 0.80 1.80384 33.89 18 144.9113 0.10 19 13.1441 2.701.61800 63.33 20 −300.7928 7.20 21 −38.5116 0.80 1.80610 40.92 22 7.08743.50 1.62004 36.26 23 −15.7257 2.00 24 −8.3980 1.20 1.75500 52.32 25−14.8336 (d25) 26 0.0000 1.00 1.51680 64.12 27 0.0000 1.50 28 0.00001.87 1.51680 64.12 29 0.0000 0.40 30 0.0000 0.70 1.51680 64.12 31 0.0000(Bf) Focal length of lens group Group Initial surface Focal length 1 159.4437 2 6 −12.0481 3 14 14.3179

In Example 3, the axial air space d5 between the first and second lensgroups G1, G2, the axial air space d12 between the second and third lensgroups G2, G3, the axial air space d25 between the third lens group G3and filter group FL, and the back focus Bf vary during zooming. Thefollowing Table 8 lists variable spaces at infinity at respective focallengths in the wide-angle end, intermediate focal length, and telephotoend states.

TABLE 8 W IF T f 29.5364 65.4997 107.0894 d5 2.0000 19.6062 25.1011 d129.1910 4.7496 1.5000 d25 16.9515 23.3655 31.0414 Bf 0.4999 0.4999 0.4998

The following Table 9 lists values corresponding to the conditionalexpressions in Example 3.

TABLE 9 fw = 29.5364 f1 = 59.4437 f1a = 252.1944 f1b = 76.9230 f2 =−12.0481 f3 = 14.3179 (1)f1b/f1a = 0.3050 (2)f1/fw = 2.0126 (3)f1b/f1 =1.2940 (3)f1/(−f2) = 4.9339 (3)f1/f3 = 4.1517

FIGS. 7A to 7C are aberration charts showing various aberrations ofExample 3 at d-line (λ=587.6 nm). FIG. 7A is an aberration chart uponfocusing at infinity in the wide-angle end state (f=29.54 mm). FIG. 7Bis an aberration chart upon focusing at infinity in the intermediatefocal length state (f=65.50 mm). FIG. 7C is an aberration chart uponfocusing at infinity in the telephoto end state (f=107.09 mm). Theaberration charts indicate that various aberrations are favorablycorrected in each focal length state from the wide-angle end state tothe telephoto end state, whereby Example 3 has excellent imagingperformances.

Example 4

FIG. 8 is a view showing the structure of the zoom lens system ZL4 inaccordance with Example 4 of the present invention. In the zoom lenssystem ZL4 of FIG. 8, the first lens group G1 is composed, in order fromthe object, of a first-a partial lens group G1 a and a first-b partiallens group G1 b; the first-a partial lens group G1 a is made of acemented positive lens constructed by cementing a negative meniscus lensL11 having a convex surface facing the object and a double convex lensL12 together; and the first-b partial lens group G1 b is constituted bya double convex lens L13. The second lens group G2 is composed, in orderfrom the object, of a double concave lens L21, a cemented negative lensconstructed by cementing a double concave lens L22 and a negativemeniscus lens L23 having a concave surface facing the image together,and a double concave lens L24. The third lens group G3 is composed, inorder from the object, of a third-a partial lens group G3 a and athird-b partial lens group G3 b; the third-a partial lens group G3 a iscomposed of a double convex lens L31, a cemented positive lensconstructed by cementing a double convex lens L32 and a double concavelens L33 together, and a double convex lens L34; and the third-b partiallens group G3 b is composed of a cemented negative lens constructed bycementing a double concave lens L35 and a double convex lens L36together and a negative meniscus lens L37 having a concave surfacefacing the object. Further, a filter group FL is constructed by alow-pass filter, an infrared cut filter, and the like. An aperture stopS is arranged closest to the object in the third lens group G3, andmoves together with the third lens group G3 at the time of zooming fromthe wide-angle end state to the telephoto end state.

The following Table 10 lists values of data in Example 4.

TABLE 10 W IF T f = 30.00 ~ 65.50 ~ 107.09 F. NO = 4.10 ~ 4.80 ~ 5.66 2ω= 31.94 ~ 14.24 ~ 8.79 IH = 8.50 ~ 8.50 ~ 8.50 TLL = 74.85 ~ 94.77 ~104.64 s r d n ν 1 193.2233 0.95 1.83400 37.16 2 47.3650 3.00 1.4978282.52 3 −75.6262 4.20 4 42.0254 2.37 1.49782 82.52 5 −578.3692 (d5) 6−94.6162 0.80 1.69680 55.53 7 34.4303 0.87 8 −43.1620 0.80 1.69680 55.539 14.6962 2.05 1.84666 23.78 10 184.3492 1.00 11 −20.2434 0.80 1.7291654.68 12 278.2271 (d12) 13 0.0000 0.50 (aperture stop S) *14 45.29422.31 1.59201 67.02 15 −24.2906 0.10 16 16.7868 3.15 1.49700 81.54 17−21.5682 0.80 1.80384 33.89 18 29.0872 0.10 19 14.9282 2.70 1.6180063.33 20 −59.7605 7.84 21 −51.0971 0.80 1.74400 44.79 22 7.1372 3.291.61293 37.00 23 −26.5759 2.50 24 −8.0713 1.01 1.75500 52.32 25 −11.6918(d25) 26 0.0000 1.00 1.51680 64.12 27 0.0000 1.50 28 0.0000 1.87 1.5168064.12 29 0.0000 0.40 30 0.0000 0.70 1.51680 64.12 31 0.0000 (Bf) Focallength of lens group Group Initial surface Focal length 1 1 61.1194 2 6−12.1826 3 14 14.2210

In Example 4, the surface No. 14 is formed aspherical. The followingTable 11 shows data of the aspherical surface, i.e., values of theapical radius of curvature R, conical constant κ, and aspheric constantsA4 to A10.

TABLE 11 [Surface No. 14] R κ A4 A6 A8 A10 45.2942 −6.9268 −1.1290E−5−7.6188E−8 +1.4298E−9 −1.7925E−11

In Example 4, the axial air space d5 between the first and second lensgroups G1, G2, the axial air space d12 between the second and third lensgroups G2, G3, the axial air space d25 between the third lens group G3and filter group FL, and the back focus Bf vary during zooming. Thefollowing Table 12 lists variable spaces at infinity at respective focallengths in the wide-angle end, intermediate focal length, and telephotoend states.

TABLE 12 W IF T f 30.0000 65.4998 107.0895 d5 2.0000 20.2978 26.0910 d129.0187 4.7480 1.5000 d25 15.9456 21.8209 29.1420 Bf 0.4912 0.5021 0.5108

The following Table 13 lists values corresponding to the conditionalexpressions in Example 4.

TABLE 13 fw = 30.0001 f1 = 61.1194 f1a = 260.4946 f1b = 78.8004 f2 =−12.1826 f3 = 14.2210 (1)f1b/f1a = 0.3025 (2)f1/fw = 2.0373 (3)f1b/f1 =1.2893 (4)f1/(−f2) = 5.0169 (5)f1/f3 = 4.2978

FIGS. 9A to 9C are aberration charts showing various aberrations ofExample 4 at d-line (λ=587.6 nm). FIG. 9A is an aberration chart uponfocusing at infinity in the wide-angle end state (f=30.00 mm). FIG. 9Bis an aberration chart upon focusing at infinity in the intermediatefocal length state (f=65.50 mm). FIG. 9C is an aberration chart uponfocusing at infinity in the telephoto end state (f=107.09 mm). Theaberration charts indicate that various aberrations are favorablycorrected in each focal length state from the wide-angle end state tothe telephoto end state, whereby Example 4 has excellent imagingperformances.

Example 5

FIG. 10 is a view showing the structure of the zoom lens system ZL5 inaccordance with Example 5 of the present invention. In the zoom lenssystem ZL5 of FIG. 10, the first lens group G1 is composed, in orderfrom the object, of a first-a partial lens group G1 a and a first-bpartial lens group G1 b; the first-a partial lens group G1 a isconstituted by a double convex lens L11; and the first-b partial lensgroup G1 b is made of a cemented positive lens constructed by cementinga negative meniscus lens L12 having a concave surface facing the objectand a double convex lens L13 together. The second lens group G2 iscomposed, in order from the object, of a negative meniscus lens L21having a convex surface facing the object, a cemented negative lensconstructed by cementing a double concave lens L22 and a double convexlens L23 together, and a negative meniscus lens L24 having a concavesurface facing the object. The third lens group G3 is composed, in orderfrom the object, of a third-a partial lens group G3 a and a third-bpartial lens group G3 b; the third-a partial lens group G3 a is composedof a double convex lens L31, a cemented negative lens constructed bycementing a double convex lens L32 and a double concave lens L33together, and a double convex lens L34; and the third-b partial lensgroup G3 b is composed of a cemented negative lens constructed bycementing a double concave lens L35 and a double convex lens L36together and a negative meniscus lens L37 having a concave surfacefacing the object. Further, a filter group FL is constructed by alow-pass filter, an infrared cut filter, and the like. An aperture stopS is arranged closest to the object in the third lens group G3, andmoves together with the third lens group G3 at the time of zooming fromthe wide-angle end state to the telephoto end state.

The following Table 14 lists values of data in Example 5.

TABLE 14 W IF T f = 30.00 ~ 65.50 ~ 107.09 F. NO = 4.11 ~ 4.72 ~ 5.63 2ω= 31.94 ~ 14.25 ~ 8.79 IH = 8.50 ~ 8.50 ~ 8.50 TLL = 75.50 ~ 95.02 ~104.52 s r d n ν 1 227.3101 1.62 1.51680 64.10 2 −227.3101 4.72 339.0309 0.80 1.78470 26.29 4 27.4849 3.00 1.49782 82.52 5 −296.1941 (d5)6 176.0290 0.80 1.69680 55.53 7 23.2355 1.15 8 −31.8792 0.80 1.6968055.53 9 18.2337 1.96 1.84666 23.78 10 −194.3960 1.00 11 −17.4270 0.801.72916 54.68 12 −262.9406 (d12) 13 0.0000 0.50 (aperture stop S) 14148.4542 2.17 1.60300 65.44 15 −21.3098 0.10 16 21.4676 3.22 1.4970081.54 17 −15.4535 0.80 1.80384 33.89 18 86.3565 0.10 19 14.5468 2.701.61800 63.33 20 −94.3058 8.91 21 −30.7082 0.89 1.74400 44.79 22 7.28203.50 1.61293 37.00 23 −16.5601 1.29 24 −8.4090 1.01 1.75500 52.32 25−13.6611 (d25) 26 0.0000 1.00 1.51680 64.12 27 0.0000 1.50 28 0.00001.87 1.51680 64.12 29 0.0000 0.40 30 0.0000 0.70 1.51680 64.12 31 0.0000(Bf) Focal length of lens group Group Initial surface Focal length 1 163.8324 2 6 −12.6553 3 14 14.8909

In Example 5, the axial air space d5 between the first and second lensgroups G1, G2, the axial air space d12 between the second and third lensgroups G2, G3, the axial air space d25 between the third lens group G3and filter group FL, and the back focus Bf vary during zooming. Thefollowing Table 15 lists variable spaces at infinity at respective focallengths in the wide-angle end, intermediate focal length, and telephotoend states.

TABLE 15 W IF T f 30.0001 65.5003 107.0906 d5 2.0000 20.6855 20.3023 d129.6995 5.0515 1.5000 d25 15.9954 21.4733 28.9089 Bf 0.5001 0.5002 0.5002

The following Table 16 lists values corresponding to the conditionalexpressions in Example 5.

TABLE 16 fw = 30.0001 f1 = 63.8324 f1a = 220.1876 f1b = 87.7682 f2 =−12.6553 f3 = 14.8909 (1)f1b/f1a = 0.3986 (2)f1/fw = 2.1277 (3)f1b/f1 =1.3750 (4)f1/(−f2) = 5.0439 (5)f1/f3 = 4.2867

FIGS. 11A to 11C are aberration charts showing various aberrations ofExample 5 at d-line (λ=587.6 nm). FIG. 11A is an aberration chart uponfocusing at infinity in the wide-angle end state (f=30.00 mm). FIG. 11Bis an aberration chart upon focusing at infinity in the intermediatefocal length state (f=65.50 mm). FIG. 11C is an aberration chart uponfocusing at infinity in the telephoto end state (f=107.09 mm). Theaberration charts indicate that various aberrations are favorablycorrected in each focal length state from the wide-angle end state tothe telephoto end state, whereby Example 5 has excellent imagingperformances.

Example 6

FIG. 12 is a view showing the structure of the zoom lens system ZL6 inaccordance with Example 6 of the present invention. In the zoom lenssystem ZL6 of FIG. 12, the first lens group G1 is composed, in orderfrom the object, of a first-a partial lens group G1 a and a first-bpartial lens group G1 b; the first-a partial lens group G1 a is made ofa cemented positive lens constructed by cementing a negative meniscuslens L11 having a convex surface facing the object and a double convexlens L12 together; and the first-b partial lens group G1 b isconstituted by a positive meniscus lens L13 having a convex surfacefacing the object. The second lens group G2 is composed, in order fromthe object, of a cemented negative lens constructed by cementing anegative meniscus lens L21 having a concave surface facing the objectand a double concave lens L22 together and a negative meniscus lens L23having a concave surface facing the object. The third lens group G3 iscomposed, in order from the object, of a third-a partial lens group G3 aand a third-b partial lens group G3 b; the third-a partial lens group G3a is composed of a double convex lens L31, a cemented negative lensconstructed by cementing a double convex lens L32 and a double concavelens L33 together, and a double convex lens L34; and the third-b partiallens group G3 b is composed of a cemented negative lens constructed bycementing a double concave lens L35 and a double convex lens L36together and a negative meniscus lens L37 having a concave surfacefacing the object. Further, a filter group FL is constructed by alow-pass filter, an infrared cut filter, and the like. An aperture stopS is arranged closest to the object in the third lens group G3, andmoves together with the third lens group G3 at the time of zooming fromthe wide-angle end state to the telephoto end state.

The following Table 17 lists values of data in Example 6.

TABLE 17 W IF T f = 30.00 ~ 66.44 ~ 107.09 F. NO = 4.16 ~ 4.89 ~ 5.68 2ω= 31.94 ~ 14.05 ~ 8.79 IH = 8.50 ~ 8.50 ~ 8.50 TLL = 75.00 ~ 95.74 ~105.00 s r d n ν 1 273.7117 0.95 1.83400 37.16 2 55.6806 3.00 1.4978282.52 3 −68.2296 4.57 4 40.7804 2.21 1.49782 82.52 5 389.8809 (d5) 6−37.6582 1.92 1.84666 23.78 7 −13.8724 0.80 1.56384 60.66 8 24.1738 1.699 −13.0806 0.80 1.62041 60.29 10 −322.7438 (d10) 11 0.0000 0.50(aperture stop S) 12 48.0311 2.08 1.49700 81.54 13 −33.8610 0.10 1426.7689 3.28 1.60300 65.44 15 −12.8497 0.80 1.80384 33.89 16 339.19660.10 17 14.2282 2.70 1.61800 63.33 18 −74.4328 6.70 19 −60.3246 0.801.83481 42.71 20 6.9024 3.50 1.62004 36.26 21 −15.8495 1.20 22 −8.85291.20 1.78800 47.37 23 −16.7933 (d23) 24 0.0000 1.00 1.51680 64.12 250.0000 1.50 26 0.0000 1.87 1.51680 64.12 27 0.0000 0.40 28 0.0000 0.701.51680 64.12 29 0.0000 (Bf) Focal length of lens group Group Initialsurface Focal length 1 1 66.0533 2 6 −13.5128 3 12 15.2087

In Example 6, the axial air space d5 between the first and second lensgroups G1, G2, the axial air space d10 between the second and third lensgroups G2, G3, the axial air space d23 between the third lens group G3and filter group FL, and the back focus Bf vary during zooming. Thefollowing Table 18 lists variable spaces at infinity at respective focallengths in the wide-angle end, intermediate focal length, and telephotoend states.

TABLE 18 W IF T f 29.9999 66.4434 107.0887 d5 2.0000 21.6530 27.9021 d1010.2160 5.1472 1.5000 d23 17.9247 24.0759 30.7380 Bf 0.4998 0.49990.4999

The following Table 19 lists values corresponding to the conditionalexpressions in Example 6.

TABLE 19 fw = 29.9999 f1 = 66.0533 f1a = 230.0345 f1b = 91.2951 f2 =−13.5128 f3 = 15.2087 (1)f1b/f1a = 0.3969 (2)f1/fw = 2.2018 (3)f1b/f1 =1.3821 (4)f1/(−f2) = 4.8882 (5)f1/f3 = 4.3431

FIGS. 13A to 13C are aberration charts showing various aberrations ofExample 5 at d-line (λ=587.6 nm). FIG. 13A is an aberration chart uponfocusing at infinity in the wide-angle end state (f=30.00 mm). FIG. 13Bis an aberration chart upon focusing at infinity in the intermediatefocal length state (f=66.44 mm). FIG. 13C is an aberration chart uponfocusing at infinity in the telephoto end state (f=107.09 mm). Theaberration charts indicate that various aberrations are favorablycorrected in each focal length state from the wide-angle end state tothe telephoto end state, whereby Example 6 has excellent imagingperformances.

Preferably, in the optical system (zoom lens system) accordance with theembodiment, the distance (back focus) on the optical axis from theimage-side surface of the lens component arranged closest to the imageto the image surface in the shortest state is about 10 to 30 mm. In theoptical system (zoom lens system) in accordance with the embodiment, theimage height is preferably 5 to 12.5 mm, more preferably 5 to 9.5 mm.

The invention is not limited to the fore going embodiments but variouschanges and modifications of its components may be made withoutdeparting from the scope of the present invention. Also, the componentsdisclosed in the embodiments may be assembled in any combination forembodying the present invention. For example, some of the components maybe omitted from all components disclosed in the embodiments. Further,components in different embodiments may be appropriately combined.

1. A zoom lens system comprising, in order from an object: a first lensgroup having a positive refractive power; a second lens group having anegative refractive power; and a third lens group having a positiverefractive power; wherein the first lens group has a first-a partiallens group and a first-b partial lens group arranged on an image side ofthe first-a partial lens group with an air space and is constructed suchthat the first-b partial lens group moves along an optical axisdirection upon focusing from infinity to a close-range object; whereinthe third lens group comprises a third-a partial lens group having apositive refractive power and a third-b partial lens group having anegative refractive power arranged on the image side of the third-apartial lens group with an air space, and wherein the followingconditional expression is satisfied:2.0126≦f1/fw<2.6 where f1 denotes a focal length of the first lensgroup, and fw denotes a focal length of the whole system at a wide-angleend state.
 2. A zoom lens system according to claim 1, wherein thefollowing conditional expression is satisfied:0.17<|f1b|/|f1a|<0.51 where f1 a denotes a focal length of the first-apartial lens group, and flb denotes a focal length of the first-bpartial lens group.
 3. A zoom lens system according to claim 1, whereinan image-side surface of a lens component arranged closest to an imageis distanced from an image plane by at least 10 mm but not more than 30mm.
 4. A zoom lens system according to claim 1, wherein the followingconditional expression is satisfied:1.15<|f1b|/f1<1.50 where f1 denotes a focal length of the first lensgroup, and f1 b denotes a focal length of the first-b partial lensgroup.
 5. A zoom lens system according to claim 1, wherein the first-apartial lens group in the first lens group is stationary with respect toan image plane upon focusing from a close-range object to infinity.
 6. Azoom lens system according to claim 1, wherein the first-a partial lensgroup in the first lens group has a positive refractive power.
 7. A zoomlens system according to claim 1, wherein the first-b partial lens groupin the first lens group has a positive refractive power.
 8. A zoom lenssystem according to claim 1, wherein the following conditionalexpression is satisfied:2.73<f1/(−f2)<6.20 where f2 denotes a focal length of the second lensgroup.
 9. A zoom lens system according to claim 1, wherein the followingconditional expression is satisfied:2.74<f1/f3<5.14 where f3 denotes a focal length of the third lens group.10. A zoom lens system according to claim 1, wherein the third-b partiallens group in the third lens group comprises, in order from the object,a cemented negative lens and a negative lens.
 11. A zoom lens systemaccording to claim 10, wherein the negative lens in the third-b partiallens group in the third lens group is a negative meniscus lens having aconvex surface facing the image.
 12. A zoom lens system according toclaim 1, wherein at least the first and third lens groups move towardthe object upon zooming from a wide-angle end state to a telephoto endstate.
 13. A zoom lens system according to claim 1, wherein, uponzooming from a wide-angle end state to a telephoto end state, a distancebetween the first and second lens groups increases while a distancebetween the second and third lens groups decreases.
 14. An opticaldevice including the zoom lens system according to claim 1 for formingan image of the object onto a predetermined image plane.
 15. A method ofmanufacturing a zoom lens system, the method comprising the steps of:arranging, in order from an object, a first lens group having a positiverefractive power and including a first-a partial lens group and afirst-b partial lens group arranged on an image side of the first-apartial lens group with an air space, a second lens group having anegative refractive power, and a third lens group having a positiverefractive power; and verifying a focusing action of moving the first-bpartial lens group along an optical axis direction, the first-b partiallens group being adapted to focus from infinity to a close-range object;wherein the third lens group comprises a third-a partial lens group anda third-b partial lens group arranged on the image side of the third-apartial lens group with an air space; wherein the third-a partial lensgroup in the third lens group has a positive refractive power; whereinthe third-b partial lens group in the third lens group has a negativerefractive power; and wherein the following conditional expression issatisfied:2.0126≦f1/fw<2.6 where f1 denotes a focal length of the first lensgroup, and fw denotes a focal length of the whole system at a wide-angleend state.